1994A&AS..105..447H


Query : 1994A&AS..105..447H

1994A&AS..105..447H - Astron. Astrophys., Suppl. Ser., 105, 447-480 (1994/June-2)

A photometric study of β Cephei stars. II. Determination of the degrees l of pulsation modes.

HEYNDERICKX D., WAELKENS C. and SMEYERS P.

Abstract (from CDS):

The wavelength dependence of photometric amplitudes is used as a means of identifying the degrees l of pulsation modes of β Cephei stars studied in an earlier paper. To this end, an expression for the photometric amplitude of a non-rotating pulsating star is derived in terms of the wavelength of the radiation received and the degree of the pulsation mode involved. The derivation differs from earlier derivations in that the specific radiation intensity is considered instead of the outward normal radiation flux. Furthermore, the effects of the non-radial components of the Lagrangian displacement on the local surface element of the star are taken into account. The angular dependence of the specific radiation intensity is determined by a limb-darkening function. The relative Lagrangian perturbation of the specific radiation intensity is set equal to the relative Lagrangian perturbation of the outward normal radiation flux. The physical parameters of the β Cephei stars are estimated by means of calibrations of photometric systems. From a comparison of the calibrations of the Walraven, the Geneva, and the Stroemgren system for early-type stars, it appears that the most reliable values are obtained by means of the Walraven system. The influence of the uncertainties on the physical parameters on the determination of the degrees l of pulsation modes in β Cephei stars is examined. The expression for the photometric amplitude of a pulsating star is used for the determination of the degree l of a pulsation mode by fitting curves of the wavelength dependences of theoretical photometric amplitudes for various degrees l to the wavelength dependence of observationally determined photometric amplitudes. In this way, values for the degrees l of most of the pulsation modes of the β Cephei stars considered are found. It appears that not all β Cephei stars pulsate in at least one radial mode and that multiperiodic β Cephei stars pulsate in a variety of combinations of pulsation modes.

Abstract Copyright: ∼

Journal keyword(s): stars: early-type - stars: fundamental parameters - Hertzsprung-Russell (HR) diagram - stars: oscillations - stars: variables: other

Simbad objects: 62

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Number of rows : 62
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 * gam Peg bC* 00 13 14.1523490172 +15 11 00.954346538 1.75 2.61 2.84 2.94 3.13 B2IV 720 0
2 * del Cet bC* 02 39 28.9568473856 +00 19 42.631195332 2.97 3.85 4.07     B2IV 395 0
3 V* KP Per bC* 03 32 38.9776919424 +44 51 20.734775568 5.7 6.44 6.41     B2IV 133 0
4 * nu. Eri bC* 04 36 19.1419185396 -03 21 08.857744927 2.82 3.737 3.928     B2III 407 0
5 * bet CMa bC* 06 22 41.9853527 -17 57 21.307352 0.77 1.73 1.97 2.11 2.35 B1II-III 748 0
6 * ksi01 CMa bC* 06 31 51.3662820799 -23 25 06.319934859 3.10 4.09 4.33 4.45 4.72 B0.7IV 336 0
7 * 15 CMa bC* 06 53 32.9069226414 -20 13 27.309395177 3.66 4.62 4.83 4.95 5.17 B1IV 214 0
8 * 19 Mon bC* 07 02 54.7772531316 -04 14 21.235613879 3.87 4.80 5.00 5.06 5.25 B2Vn(e) 205 0
9 V* V350 Pup bC* 07 30 34.0740522576 -34 05 26.146528476 6.7 7.55 7.62     B1/2Ib/II 48 0
10 V* PT Pup bC* 07 36 41.0352383592 -19 42 08.425020168 4.65 5.524 5.699     B2III 155 0
11 V* QS Pup bC* 07 49 12.8625152304 -46 51 27.787514724 4.82 5.662 5.805     B2III 79 0
12 V* QU Pup bC* 07 51 40.3580164320 -42 53 17.533822092 4.98 5.847 6.032     B2III 62 0
13 V* V372 Car bC* 07 52 29.7416381280 -54 22 01.788879000 4.64 5.529 5.680     B2IV 85 0
14 V* IS Vel bC* 08 09 43.1541985440 -47 56 13.890437304 4.12 5.017 5.217     B2V 98 1
15 V* KK Vel bC* 09 07 42.5207085395 -44 37 56.750000545 6.03 6.76 6.80     B2II/III 68 0
16 V* IL Vel bC* 09 17 31.1516725008 -52 50 19.476373704 8.51 9.13 9.16     B2III 44 0
17 HD 90288 bC* 10 23 56.9130221208 -57 27 52.421282964 7.05 8.02 8.17     B2III/IV 42 0
18 V* V400 Car bC* 10 34 48.6840712008 -58 09 01.177020288 8.93 9.75 9.66 10.02 11.681 OB 59 0
19 V* V401 Car bC* 10 35 30.0530262192 -58 12 08.180867304 8.83 9.57 9.50 9.89 9.36 B5 64 0
20 V* V403 Car bC* 10 35 40.7035044864 -58 12 44.280907776 7.93 8.75 8.73 9.48 8.65 B1III 63 1
21 CD-57 3347 bC* 10 35 43.2986203224 -58 13 33.642743412 9.13 9.88 9.85 9.76 9.67 B1.5III 41 0
22 V* V405 Car s*b 10 35 48.2142075456 -58 12 33.202086660 8.35 9.234 9.242 9.772 9.19 B0Iab 66 0
23 MCW 1182 bC* 10 35 48.2508447536 -58 14 16.579582539 8.36 9.37 9.23 9.26 9.21 B2.5V 39 0
24 NGC 3293 OpC 10 35 50.3 -58 14 04           ~ 327 0
25 CPD-57 3517 Pu* 10 35 53.6409550056 -58 14 47.852298744 8.44 9.26 9.22 9.13 9.05 B1V 44 0
26 V* V406 Car bC* 10 35 57.8106305760 -58 12 21.308777280 8.39 9.22 9.26 9.24 9.20 B1V 45 0
27 V* V379 Car Pu* 10 35 58.4856856776 -58 14 15.020184408 7.46 8.45 8.30 9.27 8.34 B1III 47 1
28 HD 92007 Pu* 10 36 01.5932715912 -58 15 09.587110032 8.26 9.00 8.92 9.57 8.74 B1III 76 0
29 HD 92024 Pu* 10 36 08.3339354160 -58 13 04.358647920 8.11 8.90 9.00 9.63 8.94 B1III 71 0
30 * bet Cru bC* 12 47 43.26877 -59 41 19.5792 0.03 1.02 1.25 1.38 1.64 B1IV 360 1
31 NGC 4755 OpC 12 53 39.2 -60 22 07           ~ 300 0
32 CPD-59 4564 bC* 12 53 57.5386794336 -60 24 58.092625152 8.45 9.12 9.06 9.64   B2III 65 0
33 V* V856 Cen bC* 12 57 36.2574706704 -49 46 50.094145848 7.66 8.36 8.33     B2II/III 49 0
34 * alf Vir bC* 13 25 11.57937 -11 09 40.7501 -0.20 0.74 0.97 1.06 1.30 B1V 877 1
35 * eps Cen bC* 13 39 53.25774 -53 27 59.0081 1.16 2.08 2.30 2.45 2.70 B1III 259 0
36 * bet Cen bC* 14 03 49.40535 -60 22 22.9266     0.58     B1III 371 0
37 * tau01 Lup bC* 14 26 08.2244287979 -45 13 17.123883210 3.68 4.393 4.553     B2IV 158 0
38 * alf Lup bC* 14 41 55.7557866 -47 23 17.515486 1.22 2.126 2.286     B1.5III 247 0
39 V* BU Cir bC* 14 45 10.9595976864 -55 36 05.906309508 5.23 6.016 6.089     B2III 103 0
40 V* V836 Cen bC* 14 46 25.7601403800 -37 13 20.082887904 7.04 7.88 8.05     B2 124 0
41 * del Lup bC* 15 21 22.3138254072 -40 38 51.109328940 2.12 2.995 3.190     B1.5IV 230 0
42 V* V349 Nor bC* 16 15 26.4194409792 -52 55 14.518386840 8.34 8.921 8.770     B2II/III 38 0
43 * sig Sco bC* 16 21 11.3157134 -25 35 34.051476 2.32 3.02 2.89 1.69 1.58 B1III+B1:V 898 0
44 HD 147985 bC? 16 26 56.7425350368 -43 47 57.155390448 7.45 8.03 7.92     B1/2II/III 35 0
45 V* V945 Sco bC* 16 53 54.5203569984 -41 52 14.960561412 9.090 9.745 9.575 9.618 9.260 B1V 45 0
46 V* V1032 Sco bC* 16 53 58.6055666592 -41 48 41.790648132 9.327 9.920 9.767 9.811 9.445 B2V 42 0
47 V* V946 Sco bC* 16 54 01.7631666120 -41 51 11.868345252 9.890 10.471 10.281 10.327 9.927 B2IV-V 49 0
48 NGC 6231 OpC 16 54 14.4 -41 48 53           ~ 562 0
49 V* V964 Sco bC* 16 54 18.3200772432 -41 51 35.651104416 9.126 9.776 9.603 9.61 9.290 B0.5V 63 0
50 V* V947 Sco bC* 16 54 36.0500878224 -41 53 38.119259292 9.45 10.06 9.78 10.06   B1V 53 0
51 CPD-41 7755 Y*? 16 54 39.8785805856 -41 53 38.480359596 9.675 10.273 10.068 11.4 9.705 B1V 39 0
52 V* V920 Sco bC* 16 54 43.1657949576 -41 49 35.456774916 9.153 9.795 9.601 9.95 9.256 B1V 67 0
53 HD 156662 bC? 17 21 06.0895034592 -45 58 55.615119960 7.35 9.15 9.13 8.70   B2III 39 0
54 * tet Oph bC* 17 22 00.5793468 -24 59 58.366974 2.18 3.03 3.26 3.38 3.58 OB 350 0
55 * lam Sco bC* 17 33 36.52012 -37 06 13.7648 0.52 1.49 1.63     B2IV+DA7.9 404 0
56 * kap Sco bC* 17 42 29.27520 -39 01 47.9391 1.32 2.211 2.386     B1.5III 250 0
57 V* V2052 Oph bC* 17 56 18.4001168880 +00 40 13.273317228 5.28 5.874 5.820     B3III 222 0
58 V* BW Vul bC* 20 54 22.3947588600 +28 31 19.190976132 5.47 6.40 6.54     B2IIIv 301 0
59 * bet Cep bC* 21 28 39.5968513 +70 33 38.574681 2.05 3.01 3.23 3.33 3.55 B0.5IIIs 756 0
60 V* HN Aqr bC* 22 37 38.2846689672 -18 39 51.268772880   11.293 11.426 11.813   B 70 0
61 * 12 Lac bC* 22 41 28.6495065456 +40 13 31.609736580 4.24 5.080 5.229     B1.5III 369 0
62 * 16 Lac bC* 22 56 23.6299283136 +41 36 13.948480440 4.61 5.436 5.587     B2IVs 325 0

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